For each point considered, the low-energy SUSY parameters were obtained using SuSpect [1]}.
In what concerns the evolution of the soft-breaking right-handed sneutrino masses \(m_{\tilde{\nu }^c}^2\) , we
have assumed that the latter hardly run between the GUT scale and the low-energy one.
The flavour-violating charged
slepton parameters (e.g. \((\Delta m_{\widetilde{L}}^2)_{ij}\)  or \(\xi \) ), were estimated at the
leading order using Eq. (REF ). Concerning NUHM, we use the same value of \(\xi \)  as for CMSSM-A. Here, we
are particularly interested to study the effect of light CP-odd Higgs boson and this naive
approximation will serve our purpose. Furthermore, we use the mass insertion approximation,
assuming that mixing between left and right chiral
slepton states are relatively small. In computing the branching fractions and the
flavour violating factor \(\kappa ^E_{ij}\) 
we have assumed (physical) right-handed sneutrino masses
\(M_{\widetilde{\nu }^c} \approx 3\)  TeV and \(\left(Y_\nu ^{\dagger }Y_\nu \right) = 0.7\) , in agreement with low-energy neutrino data as well as other low-energy constraints, which are particularly relevant in the inverse seesaw case such as Non-Standard Neutrino Interactions bounds [2]}. Moreover, in our numerical analysis, we have
fixed the trilinear soft breaking parameter \(A_\nu = - 500\)  GeV (at the SUSY scale).
